Vorticity components from a gradient field #
The weak vorticity of a gradient field and its antisymmetric matrix. The antisymmetric part
∂ᵢ uₖ - ∂ₖ uᵢ of the gradient is a signed vorticity component; this is the curl input of the
div–curl recovery in thm:vorticity-regularity.
def
ESS.vorticityCurl
(G : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ)
(l : Fin 3)
(z : CKN.Foundation.Parabolic.Vec3 × ℝ)
:
The vorticity of a space-time gradient field G i j = ∂ⱼ uᵢ.
Equations
- ESS.vorticityCurl G l z = ESS.weakVorticity (fun (z : CKN.Foundation.Parabolic.ParabolicPoint) (i j : Fin 3) => G i j z) z l
Instances For
The coefficients of the antisymmetric matrix.
Equations
- ESS.vorticityEps i k l = ESS.vorticityAntisym (fun (m : Fin 3) => if m = l then 1 else 0) i k
Instances For
theorem
ESS.vorticityAntisym_curl
(G : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ)
(z : CKN.Foundation.Parabolic.Vec3 × ℝ)
(i k : Fin 3)
:
The antisymmetric matrix of the vorticity is the antisymmetric part of the gradient.
The antisymmetric matrix is linear in the vector.
theorem
ESS.vorticityCurl_sq_le
(G : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ)
(z : CKN.Foundation.Parabolic.Vec3 × ℝ)
(l : Fin 3)
:
The squared vorticity is bounded by four times the squared gradient.